G. Parente
University of Santiago de Compostela
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Featured researches published by G. Parente.
Nuclear Physics | 2000
A.L. Kataev; G. Parente; Aleksander V. Sidorov
Abstract A detailed next-to-next-to-leading order (NNLO) QCD analysis is performed for the experimental data of the CCFR collaboration for the xF 3 structure function. Theoretical ambiguities of the results of our NNLO fits are estimated by application of the Pade resummation technique and variation of the factorization and renormalization scales. The NNLO and N 3 LO α s ( Q 2 ) MS -matching conditions are used. In the process of the fits we are taking account of twist-4 1/ Q 2 -terms. We found that the amplitude of the x-shape of the twist-4 factor is decreasing in NLO and NNLO, though some remaining twist-4 structure seems to retain in NNLO in the case when only statistical uncertainties are taken into account. The question of the stability of these results to the application of the [0/2] Pade resummation technique is considered. Our NNLO results for α s ( M Z ) values, extracted from the CCFR xF 3 data, are α s ( M Z )=0.118±0.002(stat)±0.005(syst)±0.003(theory) provided the twist-4 contributions are fixed through the infrared renormalon model and α s ( M Z )=0.121 +0.007 −0.010 (stat)±0.005(syst)±0.003(theory) provided the twist-4 terms are considered as free parameters.
Physics Letters B | 1998
Andrei L. Kataev; A. V. Kotikov; G. Parente; Aleksander V. Sidorov
Abstract We present the results of the next-to-next-to-leading order QCD analysis of the recently revised experimental data of the CCFR collaboration for the xF 3 structure function using the Jacobi polynomial expansion method. The effects of the higher twist contributions are included into the fits following the infrared renormalon motivated model. The special attention is paid to the checks of the predictive abilities of the infrared renormalon model and to the independent extractions of the x -dependent shape of the twist-4 contributions to the xF 3 structure function in the process of the leading order, next-to-leading order and next-to-next-to-leading order fits of the revised CCFR data. We stress that at the next-to-next-to-leading order the results for α s ( M Z ) turn out to be almost nonsensitive to the higher-twist terms. We obtain the following result α s NNLO ( M Z )=0.117±0.002(stat)±0.005(syst)±0.003(theory). The comparison of the outcomes of our next-to-leading order and next-to-next-to-leading order analysis indicate that the theoretical QCD uncertainties were underestimated in the process of the next-to-leading order determination of α s ( M Z ), made recently by the CCFR collaboration itself.We present the results of the next-to-next-to-leading order QCD analysis of the recently revised experimental data of the CCFR collaboration for the
Physics Letters B | 1996
Andrei L. Kataev; A. V. Kotikov; G. Parente; Aleksander V. Sidorov
xF_3
Physics Letters B | 1996
A.V. Kotikov; G. Parente
structure function using the Jacobi polynomial expansion method. The effects of the higher twist contributions are included into the fits following the infrared renormalon motivated model. The special attention is paid to the checks of the predictive abilities of the infrared renormalon model and to the independent extraction of the
Physics Letters B | 2003
A.L. Kataev; G. Parente
x
Nuclear Physics | 2000
A.L. Kataev; G. Parente; Aleksander V. Sidorov
-shape of the twist-4 contributions to the
Physics Letters B | 2001
J.A. Castro Pena; G. Parente; E. Zas
xF_3
arXiv: High Energy Physics - Phenomenology | 1998
Andrei L. Kataev; A. V. Kotikov; G. Parente; Aleksander V. Sidorov
structure function in the process of the leading order, next-to-leading order and next-to-next-to-leading order fits of the revised CCFR data. We stress that at the next-to-next-to-leading order the results for
Journal of Physics G | 2003
A. L. Kataev; G. Parente; Aleksander V. Sidorov
\alpha_s(M_Z)
arXiv: High Energy Physics - Phenomenology | 1999
Andrei L. Kataev; G. Parente; Aleksander V. Sidorov
turn out to be almost nonsensitive to the higher-twist terms. We obtain the following result